Alberto P. Guimarães, Centro Brasileiro de Pesquisas Físicas …ebm/ix/arquivos/P13.pdf · 2014....
Transcript of Alberto P. Guimarães, Centro Brasileiro de Pesquisas Físicas …ebm/ix/arquivos/P13.pdf · 2014....
Magnetic vortices, skyrmions, etc.
Alberto P. Guimarães,
Centro Brasileiro de Pesquisas Físicas (CBPF),
Rio de Janeiro, Brazil
08/11/2013
IX Escola Brasileira de Magnetismo
Collaborators
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Dr. F. Garcia (CBPF), Brazil
Dr. J.P. Sinnecker (CBPF), Brazil
E.R.P. Novais (CBPF), Brazil
H.V.Cotrina (CBPF), Brazil
G.B.M. Fior (LNLS), Brazil
Outline
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1. Solitons and magnetic vortices
2. Topological properties of vortices, etc
3. Formation of a skyrmion
Solitons
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Solitons are collective excitations that are solutions of differential equations
Topological solitons (or topological defects): those whose stability is guaranteed topologically
John Scott Russell (1808–1882)
Waves in a narrow channel travel long distances without changing their shape
J. S. Russell, Report of the Fourteenth Meeting of the British Association for the Advancement of Science (Murray, London, 1844), pp. 311-390.
Examples of solitons
5http://www.youtube.com/watch?v=Ud7STKWNmQw
Solitons in a one-dimensional magnet
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a) Dynamic soliton: topologically unstable, since curve a on the sphere can be deformed continuously to a point (the ground state)(these configurations are said to be topologically equivalent)
b) Topological soliton: curve b cannot be deformed to a point
Kosevich Phys. Repts. 194, 117 (1990).)
Real systems
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Two configurations are topologically equivalent when they can transformed into one another without overcoming an infinite energy barrier
Considerations:
a) In real systems, the energy barriers are not infinite;
b) Real systems have finite dimensions, therefore, e.g., one can always expel a domain wall from a sample
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Spin structures in nanoobjects
Schematic curve of coercivity vs. diameter for soft magnetic particles.
1 2 3 4
Four regimes:
1) superparamagnetic;
2) single-domain FM;
3) vortex state;
4) multidomain FM
Properties of magnetic vortices
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Shinjo et.al., Science 289, 930 (2000)
Computed vortex and core profile Bode, PRL 100, 029703 (2008)
Pigeau
Circular nanodots:phasediagram
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Different spin
configurations
Graph:
Height vs. thickness
Novais JAP 110, 053917 (2011)
Micromagnetic simulations
The properties of nanoscopic or microscopic magnetic samples may be
simulated numerically. In the Micromagnetism approach, the magnetic
medium is treated as a continuum.
The total energy is a sum of the terms of exchange, anisotropy,
magnetostatic and Zeeman:
The spin configuration is found by minimizing the total energy Etot
or
Formation of a vortex on a permalloy nanodisk
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Properties of magnetic vortices
• Circulation:
c=-1 (CW)c=+1 (CCW)
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Combining c and p:
chirality or handedness:cp= 1
• Polarity:
p=-1p=+1
a. Applications of vortex systems:Vortex Random-access Memory
(VRAM)
e.g. Bohlens, Appl. Phys. Lett. 93, 142508 (2008)
Vortices may store 1 bit using
a) Polarityb) Circulation (CW or CCW) c) Chirality
Or else store 2 bits using, e.g.,
a) Polarity and circulation
b. Applications of vortex systems : spin torque nano-oscillators (STNOs)
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Polarized spin currents can induce periodic motion of vortex cores (gyrotropic motion), also emitting RF
(Pufall 2007, Mistral 2008)
Coupling of vortices in spin valve nanopillar may increase rf power
Mistral PRL 100 257201 (2008)
c. Applications of vortex systems : destruction of cancer cells
Kim, Nature Mater. 9 165, (2010)
Torque =m×H
Oscillation of the disks induces programmed cell death
d. Applications of vortex systems: logic gates
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The output of the center disk is controlled by the input to disks 1 and 3
Gyrotropic motion of vortex cores
The vortex core performs a spiral-like motion with a frequency related to the disk aspect ratio β=h/R
The direction of the translation is defined by the polarity p (up or down)
Gyrotropic motion of a vortex core
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Translation motion of magnetic vortex core displaced from the equilibrium position (zero damping)
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The vortex core motion of a inhomogeneous assembly of nanodisks produces an echo that may be used to characterize it
This is analogous to the NMR spin echo
The evolution of the total magnetization
Projection of the image of the disks
Superposed image of several disks
Topology?!
21Remember: in topological terms, one coffee cup=one donut
Jwilson.coe.uga.edu
Winding number
22Braun Adv. Phys. 61, 1–116 (2012)
One cannot deform a given spin configuration into another of different winding number
A topological defect exists if one cannot deform a spin configuration into the ferromagnetic state
The winding number is the total variation of the magnetization angle ∆ as one moves counterclockwise around a circle, divided by 2
Vortices and antivortices
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AntivortexVortex
n=1 n=-1
p=±1 p=±1
When a vortex and an antivortex meet, they annihilate.
Winding number n and skyrmion number q
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The winding number: total variation of the magnetization angle ∆ as one moves counterclockwise around a circle divided by 2
The winding number of a vortex is 1
The skyrmion number q is
where p is the polarity
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Vortex and antivortex
When the sum of the skyrmionnumbers of the vortex and the antivortex is not zero, the annihilation releases a burst of energy
Annihilation of a vortex and the conservation of the skyrmion number
1D Domain walls and skyrmions
26Menzel, Thesis, Hamburg (2011)
The importance of the winding number (and the total skyrmion number S) In b) the total skyrmion number S is zeroIn c) S=1 and the one-dimensional domain walls need a higher field to be annihilated – a skyrmion is formed
2D Domain walls
Effect of applied field on domain walls with different topologies: 1) q =0, the walls disappear; 2) q ≠0 topologically protected
Kunz, APL94, 132502 (2009)
1) 2)
Edge defects in a domain wallI
n=+1/2
n=-1/2
n=-1/2
n=+1/2
This is a representation of the first stripe (previous slide)
A DW is composed of 2 ormore defects with winding numbers
+1/2 or -1/2
Opposite charges annihilate
Edge defects in a domain wall II
n=+1/2
n=-1/2
n=+1/2
n=-1/2
This is a representation of the second stripe (previous slide)
If the total charge on eachedge does not add to zero, a 360o wall is formed, and a higher field is necessary to destroy it
Charges do not add to zero
Collapse of two DWs: formation of a skyrmion
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Micromagnetic simulation of a stripe with perpendicular anisotropy, topologically protected, with increasing perpendicular applied field
Garcia, unpublished (2013)
Collapse of two DWs: formation of a skyrmion
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Collapse of two DWs: formation of a skyrmion
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Collapse of two DWs: formation of a skyrmion
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Collapse of two DWs: formation of a skyrmion
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Collapse of two DWs: formation of a skyrmion
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Collapse of two DWs: formation of a skyrmion
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Collapse of two DWs: formation of a skyrmion
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Collapse of two DWs: formation of a skyrmion
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Collapse of two DWs: formation of a skyrmion
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Collapse of two DWs: formation of a skyrmion
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Skyrmions
41T.H.R. Skyrme, Nucl. Phys. 31, 556–569 (1962).
A class of solitons found in liquid crystals, Bose-Einstein condensates, quantum Hall magnets, thin magnetic films, and materials with Dzyaloshinsky-Moriya (DM) interaction, named after T.H.R. Skyrme (1922–1987)
Skyrmion lattices and isolated skyrmions
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Skyrmion lattices:
Nanolayers of materials with intrinsic chirality (cubic helimagnetsFe0.5Co0.5Si and FeGe (Yu (2010, 2011)) and with induced chirality (Fe/W bilayers) Heinze (2011))
Isolated skyrmions:
Nanolayer of Fe0.5Co0.5Si (L = 20 nm) for H ≈ 50mT (Yu (2010, 2011).
Kiselev J. Phys. D: Appl. Phys. 44 (2011) 392001
Skyrmion phase diagram (Applied field Vs. Kappa)
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Ha=K/M
=D/4sqrt(AK)
D – Dzyaloshinsky-MoriyaCoefficient
K – anisotropy
A – exchange stiffness
Kiselev J. Phys. D: Appl. Phys. 44 (2011) 392001
Diagram for film of thickness L (fixed ratios K/M and L/WDW)(in the hatched area spatially modulated skyrmion phases are stable)
Dzyaloshinskii–Moriya interactions
44Fert 2012
Magnetic bubbles
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Cylindrical domains with perpendicular magnetization in magnetic films (e.g., of ferrite, garnet)
Bubble radius of the order of 1 micron
Applications to magnetic memories studied in the 1960s and 1970s
Wikipedia
H=0 H0
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Current-induced motion of a skyrmion on a Co stripe – low depinning currents
Creation of skyrmions
Iwasaki et al. Nat. Nano. 8 (2013)
Tuning the properties of the vortex:
Varying the Co thickness in Co/Pt multilayers, the anisotropy Kz can be increased, and the vortex core diameter also increases.
1 2 3
1.PEEM image, 2. simulation, 3. simulation
Skyrmions without DM
49Novais , unpublished (2013)
Diameter vs. stripe width
Motion of a skyrmion
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Simulation of the motion of askyrmion in a CoPt disk, with perpendicular anisotropy Kz=1.2X106 J /m3 Novais , unpublished (2013)
SummaryTopological properties of magnetic systems are relevant for their dynamic behavior
Magnetic vortices and skyrmions are topological defects
Skyrmions are stable structures, topologically protected, related to magnetic vortices and to magnetic bubbles
Skyrmions may be stable with or without DM interaction
Skyrmions may be displaced through the action of polarized currents, with much smaller current densities than domain walls
Skyrmions may have applications in memory devices51
Some general References
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A. P. Guimarães, Principles of Nanomagnetism, Springer (2009)
K. Y. Guslienko, J. Nanoscience Nanotechnol., 8 2745-2760 (2008)
A.M. Kosevich et al. Phys. Repts. 194, Nos. 3 & 4 117—238 (1990).
Menzel, Thesis, Hamburg University (2011)
Thank you!